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9 Questions around this concept.
A radioactive nuclei with a decay constant of 0.5/s is being produced at a constant rate of 100 nuclei/s. If at t = 0, there were no nuclei, the time when there are 50 nuclei is :
A radioactive nucleus undergoes a series of decay according to the scheme
If the mass number and atomic number of A are 180 and 72 respectively, these numbers of are:
The mean lives of a radioactive sample are 30 years and 60 years for - emission and
-emission
respectively. If the sample decays both by -emission and
-emission simultaneously, the time after which,
only one-fourth of the sample remains is:
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A parent radioactive nucleus (decay constant
) converts into a radio-active nucleus
of decay constant
, Initially, number of atoms of
is zero. At any time
are number of atoms of nuclei
and
respectively then maximum value of
is :
The ratio of N1 to N2 when N2 is maximum is:
At time $\mathrm{t}=0$, a material is composed of two radioactive atoms A and B, where $N_A(0)=2 N_B(0)$. The decay constant of both kind of radioactive atoms is $\lambda$. However, A disintegrates to B and B disintegrates to C . Which of the following figures represents the evolution of $N_B(t) / N_B(0)$ with respect to time t ?
$
\left[\begin{array}{l}
N_A(0)=N o . O f A \text { atoms at } t=0 \\
N_B(0)=N o . O f B \text { atoms at } t=0
\end{array}\right]
$
Two species of radioactive atoms are mixed in equal numbers. The disintegration constant of the first species is $\lambda$ and of the second is $\lambda / 3$. After a long time the mixture will behave as a species with a mean life of approximately
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As we know that due to radioactive disintegration a radio nuclide transforms into its daughter nucleus. Depending on the nuclear structure and its unstability, a parent nucleus may undergo either $\alpha-$ or $\beta-$ emission. Sometimes a parent nucleus may undergo both types of emission imultaneousonly.
If an element decays to different daughter nuclei with different decay constant $\lambda_1, \lambda_2, \lambda_3, \ldots$ etc. for each decay mode, then the effective decay constant of the parent nuclei can be given as
$
\lambda_{e f f}=\lambda_1+\lambda_2+\lambda_3, \ldots
$
Similarly, for a radioactive element with decay constant $\lambda$ which decays by both $\alpha-$ and $\beta-$ decays given that the probability
for an $\alpha$-emission is $\mathrm{P}_1$ and that for $\beta-$ emission is $\mathrm{P}_2$ the decay constant of the element can be split for individual decay modes. Like in this case the decay constants for $\alpha-$ and $\beta-$ decay separately can be given as
$
\begin{aligned}
& \lambda_\alpha=P_1 \lambda \\
& \lambda_\beta=P_2 \lambda
\end{aligned}
$
Accumulation of Radioactive element in Radioactive series-
A radioactive element decays into its daughter nuclei until a stable element appears. Consider a radioactive series-
$
A_1 \xrightarrow{\lambda_1} A_2 \xrightarrow{\lambda_2} A_3 \xrightarrow{\lambda_3} \ldots
$
A radioactive element $A_1$ disintegrates to form another radioactive element $A_2$ which in turn disintegrates to another element $A_3$ and so on. Such decays are called Series or Successive disintegration.
Here, the rate of disintegration of $A_1=$ Rate of formation of $A_2$
$
\begin{aligned}
& \frac{-d N_{A 1}}{d t}=\frac{d N_{A 2}}{d t}=\lambda_1 N_{A 1} \\
& \frac{-d N_{A 2}}{d t}=\frac{d N_{A 3}}{d t}=\lambda_2 N_{A 2} \\
& \frac{d N_{A 1}}{d t}=-\lambda_1 N_{A 1} \\
& \frac{d N_{A 2}}{d t}=-\lambda_2 N_{A 2}
\end{aligned}
$
Therefore, net formation of $A_2=$ Rate of disintegration of $A_1$ - Rate of disintegration of $A_2$
$
=\lambda_1 N_{A 1}-\lambda_2 N_{A 2}
$
If the rate of disintegration of $A_1$ becomes equal to the Rate of disintegration of $A_{2,}$ then it is called Radioactive equilibrium. So the equation becomes -
$
\Rightarrow \frac{\lambda_1}{\lambda_2}=\frac{N_{A 2}}{N_{A 1}}=\frac{T_{a v g 2}}{T_{a v g 1}}=\frac{\left(T_{\frac{1}{2}}\right)_2}{\left(T_{\frac{1}{2}}\right)_1}
$
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